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![]() Materials Sciences and Applicatio ns, 2011, 2, 638-642 doi:10.4236/msa.2011.26087 Published Online June 2011 (http://www.SciRP.org/journal/msa) Copyright © 2011 SciRes. MSA Synthesis and Magnetic Properties of Conventional and Microwave Calcined Strontium Hexaferrite Powder Kanagesan Samikannu1, Jesurani Sinnappan1,2, Sivakumar Mannarswamy1, Thirupathi Cinnasamy1, Kalaivani Thirunavukarasu1 1Center for Material Science and Nano Devices Department of Physics, SRM University, Kattankulathur, India; 2Department of Physics, Jeyaraj Annapackium College for Women, Periyakulam, India. Email: [email protected] Received December 24th, 2010; revised March 21st, 2011; accepted May 17th, 2011. ABSTRACT Powders of strontium hexaferrite (SrFe12O19-SrF) have been prepared by the sol-gel process. The prepared precursor was calcined in two different calcination techniques, using conventional furnace and microwave furnace. Thermal analysis studies showed exothermic and endothermic reaction peak at room temperature to 1200˚C. An investigation of SrFe12O19 crystalline powder from the structural and magnetic aspect is performed using X-ray diffraction (XRD), high resolution scanning electron microscopy (HR-SEM) and vibrating sample magnetometer (VSM). The average particle diagonal size of SrFe12O19 powder was 80 - 100 nm in conventional and 40 - 70 nm in microwave calcinations respec- tively. XRD result showed the formation of SrFe12O19 of the sample calcined at 900˚C with Fe/Sr: D-Fructose ratio = 12. Keywords: Sol-Gel, Strontium Hexaferrite, D-Fructose, Magnetization 1. Introduction The M-type Strontium Hexaferrite-SrFe12O19 (SrF) is a hard magnetic material due to its high coercivity. SrFe12O19 crystallize with 64 ions per unit cell on 11 dif- ferent symmetry sites, the magnetic structure given by Gorter model, 24 Fe3+ atoms are arranged over five dis- tinct sites: three octahedral sites and two tetrahedral sites. These five sites are coupled via ferromagnetic superex- change interaction through O2− ions [1]. Recently, Wang et al., reported a correlation between magnetic properties and particles morphology of SrFe12O19 [2]. By control- ling the microstructure, morphology and chemical com- position and particle size, the magnetic properties of the material can be improved. Ferrites, typically spinel ferrite and magnetoplumbite ferrite, can be used as recording materials, microwave devices, humidity sensors, pig- ments etc. Compared with spinel ferrite, magnetoplum- bite ferrites, strontium ferrite have attracted more scien- tific research in recent years due to their high uniaxial magnetic anisotropy, high saturation magnetization and high coercivity [3,4]. In order to get homogeneous ferrite, several techniques have been used in the preparation of Sr hexaferrite, such as the chemical co precipitation [5], hydrothermal [6], sol-gel [7,8], micro emulsion [9], and citrate precursor [10] have been developed. Therefore, the preparation of SrFe12O19 having high purity, ultrafine size, good dispersion and excellent magnetism has been the focus of recent research [7,11]. The growing interest during the past decade is essentially due to the fact that microwave heat treatment could influence the micro- structure can improve the material properties. Conven- tional furnace heating samples by the surface heating mechanism and depending on the rate of heating, a large thermal gradient from the surface to the centre can be generated within a sample, particularly with materials heaving a poor thermal conductivity. Microwave heating would be promising because it is a self-heating process of absorbing the electromagnetic energy. As a result of the internal and volumetric heating at high heating rate may lead to reduction in manufacturing cost on account of energy savings, shorter processing times and improved product uniformity and yields, limited grain growth throughout the ceramic body. It is well known that the heating rate and thermal efficiency of the microwave heating is higher than those of conventional method [12, 13]. In this paper, we report the preparation of SrFe12O19 ![]() Synthesis and Magnetic Properties of Conventional and Microwave Calcined Strontium Hexaferrite Powder639 by sol-gel process and important hysteresis parameters of the powders with influence of convention and microwave calcinations. 2. Experimental The powder was prepared by sol-gel technique using D-Fructose as the fuel. Analytical grade Ba(NO3)2, Fe(NO3)3·9H2O and D-Fructose were used as starting materials. Nitrate and fuel ratio is 1:1. Stoichiometric amount of metal nitrates and fuel were taken, dissolved in distilled water and stirred by magnetic stirrer for 2 h to get a solution. Sol was heated at 80˚C with stirring con- tinuously, finally it changed in to sticky liquid gel and it was preheated at 130˚C in a hot air oven for two days to get precursor. The precursor was calcined (Conventional and microwave) at 900˚C, to get crystalline barium hexaferrite powder. 2.1. Characterization Thermo gravimetric analysis of the mixture composed of barium nitrate, iron nitrate and D-Fructose (precursor) were carried out between 28˚C and 1200˚C on NETZSCH STA 409 C/CD in the static air atmosphere at the heating rate of 10˚C per minute. The DTA analyses of same mixtures were also carried out on the same instrument at same condition. The crystalline phases were identified by means of X-ray diffraction (XRD) measurements (PANa- lytical X’pert pro) CuKα radiation at 45 kV and 40 mA (λ = 0.15406 nm) in a wide range of 2θ (10˚ < 2θ < 80˚). The surface morphology and size of the ferrite particles were studied by using FEI Quanta FEG 200-High resolu- tion scanning electron microscope (HR-SEM) and Mag- netization measurements at room temperature were car- ried out on Lakeshore Vibrating Sample Magnetometer (VSM) at a maximum applied field of 15,000 Gauss at room temperature. 3. Results and Discussion The thermogram of the precursor of barium hexaferrite derived by mixing of barium nitrate, ferric nitrate and D-Fructose as shown in Figure 1. TGA shows the initial weight loss from 28˚C to 185˚C due to the loss of ab- sorbed water [14]. The subsequent loss up to 400˚C is associated mainly to the decomposition of the D-fructose. In order to verify this, separate TGA was undertaken for D-fructose, thermogram is shown in Figure 2. It shows the major weight loss between 200˚C and 400˚C thus supporting our assignment. Therefore, D-Fructose pro- vides self heat to promote the reaction and to reduce the crystallization temperature of the hexaferrite. The stage of decomposition between 400˚C and 775˚C is due to decomposition of nitrates and starting formation of hexaferrite. There is no considerable weight loss above Figure 1. TG-DTA curves for the precursor. Figure 2. TG-DTA curves for D-fructose. 900˚C, confirming the formation of the stable Strontium hexaferrite this analysis, therefore illustrates the optimum calcinations temperature for Strontium hexaferrite is around 900˚C. The sequences of reaction taking place is shown in the following steps 200C - 500C 23 PrecursorFe O+SrO 250C - 750C 23 24 Fe OSrOSrFe O above 750 C 232412 19 5Fe OSrFe OSrFeO Figure 3 shows the XRD patterns of the powders con- ventionally calcined at temperatures 500˚C, 750˚C and 900˚C for 3 h in air, respectively. The precursor is cal- cined at 500˚C; the powders can be described as Fe2O3 and SrO and then the phase of SrFe2O4 and hexagonal SrFe12O19 can been detected for samples calcined at 750˚C. Clear diffraction peak of SrFe12O19 can be ob- tained at 900˚C, which coincides with the JCPDS file Copyright © 2011 SciRes. MSA ![]() Synthesis and Magnetic Properties of Conventional and Microwave Calcined Strontium Hexaferrite Powder 640 number: 84-1531. Calcination temperature and interme- diate Fe2O3 plays an important role in the formation of Strontium Hexaferrite. The phase development micro- wave calcined powder at different temperatures, 500˚C, 750˚C and 900˚C for 10 minutes, the peaks correspond- ing to the standard diffraction pattern of SrO, SrFe2O4 and SrFe12O19 and is shown in Figure 4. In order to visualize the conventional calcined powder are in elongated hexagonal like structure, diagonal size vary in the range of 80 - 100 nm and it is not well de- fined shape (Figure 5). The HR-SEM micrograph for the microwave calcined powder at 900˚C for 10 minutes is shown in Figure 6. The particles are hexagonal platelets and well crystalline strontium ferrite, diameters are in the range of 40 nm to 70 nm. This type of shape is usually observed for BaFe12O19 or SrFe12O19 obtained by sol-gel process [4,15]. The morphology of the microwave cal- cined powder samples reveal smaller particles compared Figure 3. XRD patterns of the powders calcined at different temperatures: (a) 500˚C, (b) 750˚C, and (c) 900˚C for 3 h. Figure 4. XRD patterns of the powders microwave calcined at different temperatures: (a) 500˚C, (b) 750˚C, and (c) 900˚C for 10 minutes. Figure 5. HR-SEM image of conventionally calcined pow- der at 900˚C for 3 h. Figure 6. HR-SEM image of microwave calcined powder at 900˚C for 10 minutes. to the conventionally calcined powder. Hard magnetic materials with hexagonal structure is mainly due to the microwave energy coupled through polarization, elec- tronic and ionic conductivity loss therefore a smaller particle size resulted from the enhanced diffusion and accelerated densification [16]. Figure 7 shows the magnetization versus applied field for conventional and microwave treated samples at room temperature. The reduction in Ms in microwave calcined powder can be attributed to the decrease in the size of the particles. The observed value of saturation magnetization 47 A·m2/kg for the sample conventionally calcinated at 900˚C are far from the theoretical Ms value of 74.3 Copyright © 2011 SciRes. MSA ![]() Synthesis and Magnetic Properties of Conventional and Microwave Calcined Strontium Hexaferrite Powder641 Figure 7. Magnetization curve of SrFe12O19 (a) powder conventionally calcined at 900˚C for 3 h; (b) powder mi- crowave calcined at 900˚C for 10 minutes. A.m2/kg and the coercivity 6,709 Gauss very close to the theoretical Hc. Observed magnetization values are close to those observed in other methods of preparation (50 - 60 Am2/kg) [5,6,10,17]. The value of Mr (26.58 Am2/kg) is approximately 59% of Ms it has maximum coercivity of 6,708 Gauss for microwave calcined powder is lower than those of the literature and of the theoretical limit (7,500 Gauss) [18]. The samples calcined conventionally and microwave at 900˚C shows smooth hysteresis loop, which confirms the formation of pure strontium hexafer- rite [18,19]. 4. Conclusions The effective influence of conventional and microwave on the structure and magnetic properties crystalline SrFe12O19 are discussed. The samples were subjected to two different heat treatments. From the analysis of vari- ous characterization techniques such as XRD, HR-SEM and VSM, we observe that the structure remained intact with different heating treatment process. The possibility of lowering the synthesis temperature and get a pure SrF powder, microwaves allows the reduction of particle size in the hexaferrite. The external diameters of the obtained different method of calcined SrFe12O19 particles range between 40 to 100 nm. The results indicate that calcina- tions method has significant effect on the saturation magnetization (Ms). These magnetic materials can poten- tially be used in micro/nano electronic devices, gas sen- sors and catalysts. 5. Acknowledgements The authors thank SRM University for providing the facilities available in Nanotechnology center. REFERENCES [1] J. F. Wang, C. B. Ponton and I. R. 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